TECHNICAL FIELD
[0001] The disclosed technology relates generally to the collection of bodily fluids, and
in particular, to the devices, methods, and design principles allowing the collection
of bodily fluids into a receptacle and, in certain embodiments, the process of acting
on the fluid being collected with the utilization of gravity to add functionality.
This has implications not only for active fluid collection, but also on downstream
processing of the receptacle, including its presentation to equipment and processes.
BACKGROUND
[0002] Devices, systems and methods to collect bodily fluids are necessary devices for the
growing field of personalized medicine. As point-of-care devices continue to improve,
an often overlooked area lies within the collection of samples from untrained users.
Currently, biological samples are most commonly obtained via either simple-to-use
methods or devices, as with generic lancing devices, or trained personnel, as with
phlebotomy venipunctures. In order to transfer the bodily fluid to a container, receptacle,
or an analysis device, multiple steps are required that are time consuming and/or
cumbersome. To circumvent these problems, there is a need for devices that are able
to collect samples in a simple manner and have an integrated fluidic transfer to a
container or receptacle that houses the samples.
[0003] WO2014/088606 discloses bodily fluid sample collection systems, devices, and method.
US3623475 discloses a blood collector device.
US2013/211289 discloses a handheld device for drawing, collecting, and analyzing bodily fluid includes
a body having a lumen defined therein, a plunger configured to be user-actuated, and
a base.
US2014/038306 discloses fabricating and using open microfluidic networks according to methods,
systems, and devices that can be used in applications ranging from home-testing, diagnosis,
and research laboratories.
US2014/042094 discloses an independent blood filter device depends on flow geometry to deliver
blood serum or plasma free of detrimental levels of hemoglobin.
US2008/028821 discloses a corpuscle/plasma separating part is disposed at the lower end of the
substrate, and a sensor part connected to the corpuscle/plasma separating part is
disposed at the upper end of the substrate, with a calibration solution reservoir
being disposed on the lower side of the sensor part, and a calibration solution waste
reservoir being disposed on the upper side of the sensor part.
US2011/257498 discloses a blood test apparatus has a housing with an opening, and a plunger that
moves back and forth inside the housing, the plunger having a projecting member.
US2007/260193 discloses a safety blood collection device including holder housing adapted to maintain
a needle cannula with a puncture tip extending from a forward end thereof and to receive
a sample collection tube through a rearward end thereof.
[0004] Thus, there is a need in the art for improved microfluidic devices that utilize gravity
and capillary forces for fluid handling and transfer, and related systems and methods.
BRIEF SUMMARY
[0005] The present invention is defined with reference to the appended claims. Also discussed
herein are various embodiments of the collection device, as well as associated systems
and methods for its use. For brevity, these embodiments may be described in relation
to a "collector," though that is not intended to limit the scope of the disclosure
in any way. Further, the discussion of microfluidic channels may comprise open and
closed channels, as well as channels featuring both open and closed portions.
[0006] In Example 1, microfluidic collection system for drawing blood from a subject comprising
a collector further comprising a housing, at least one collection site, a microfluidic
network further comprising at least one microfluidic channel disposed within the housing,
and at least one outflow channel in fluidic communication with the microfluidic network,
and at least one reservoir in fluidic communication with the at least one collection
site by way of the outflow channel, wherein the system is configured to be placed
on a subject's skin to draw blood, and the at least one microfluidic network is configured
to promote the flow of fluids from the collection site to the at least one outflow
channel.
[0007] In Example 2, the system of Example 1, further comprising an actuator configured
to facilitate the puncture of skin.
[0008] In Example 3, the system of Example 1, wherein the at least one microfluidic channel
further comprises a microfluidic channel geometry and a contact angle, and further
wherein the at least one microfluidic channel is configured to promote the flow of
fluids by at least one of capillary action and gravitational force.
[0009] In Example 4, the system of Example 3, wherein the collector and at least one microfluidic
channel is configured to have a flow position and a stop position.
[0010] In Example 5, the system of Example 3, further comprising at least one open microfluidic
channel.
[0011] In Example 6, the system of Example 3, further comprising at least one open microfluidic
channel and at least one closed microfluidic channel.
[0012] In Example 7, the system of Example 3, wherein the microfluidic network further comprises
at least one ramp.
[0013] In Example 8, the system of Example 3, wherein the micro fluidic network further
comprises at least one surface tension valve.
[0014] In Example 9, the system of Example 8, wherein the surface tension valve is configured
to regulate the flow of fluids through the microfluidic network based on the orientation
of the microfluidic network.
[0015] In Example 10, the system of Example 3, further comprising a coupling portion.
[0016] In Example 11, the system of Example 10, wherein the reservoir is detachable, and
the coupling portion is further configured to receive a detachable reservoir.
[0017] In Example 12, gravity-enhanced collection system comprising a collector, further
comprising a housing, a microfluidic network, further comprising at least one microfluidic
channel disposed within the housing, at least one collection site disposed within
the housing, at least one outflow channel, and at least one reservoir, wherein the
at least one collection site is in microfluidic communication with the outflow channel
by way of the microfluidic network so as to promote the flow of fluid to the reservoir
by way of the outflow channel into the reservoir.
[0018] In Example 13, the system of Example 12, wherein the device is configured to use
gravity to enhance fluid collection.
[0019] In Example 14, the system of Example 13, wherein the reservoir is a detachable reservoir.
[0020] In Example 15, the system of Example 13, wherein the outflow channel is configured
to prevent backflow.
[0021] In Example 16, the system of Example 13, wherein the at least one microfluidic channel
further comprises an open microfluidic channel and a closed microfluidic channel in
fluidic communication with one another.
[0022] In Example 17, the system of claim 16 wherein the open microfluidic channel and closed
microfluidic channels are in fluidic communication with one another.
[0023] In Example 18, the system of claim 16 further comprising a ramp. In certain Examples,
this ramp may comprise an open microfluidic channel with at least one wetted surface
defining a wetted perimeter length, wherein the wetted surface contacts a fluid flowing
through the channel at a contact angle, and at least one free surface comprising an
open air-liquid interface defining a free perimeter length, wherein the ratio of the
free perimeter length to the wetted perimeter length is less than the cosine of the
contact angle, thereby enabling spontaneous capillary flow.
[0024] In Example 19, the system of channel 15, wherein the at least one microfluidic channel
is capable of timed fluid delivery.
[0025] In Example 20, a method of drawing blood from a subject, comprising providing a blood
collection device, comprising a housing, a microfluidic network further comprising
at least one microfluidic channel disposed within the housing and at least one collection
site, at least one outflow channel in fluidic communication with the microfluidic
network, and at least one reservoir in fluidic communication with the at least one
collection site by way of the network and outflow channel, placing the fluid connection
device on the skin of the subject, puncturing the subject's skin so as to pool fluid,
collecting pooling fluid from the skin and transporting it to the reservoir by way
of the microfluidic network.
[0026] While multiple embodiments are disclosed, still other embodiments of the disclosure
will become apparent to those skilled in the art from the following detailed description,
which shows and describes illustrative embodiments of the disclosed apparatus, systems
and methods. As will be realized, the disclosed apparatus, systems and methods are
capable of modifications in various obvious aspects. Accordingly, the drawings and
detailed description are to be regarded as illustrative in nature and not restrictive.
BRIEF DESCRIPTION OF THE DRAWINGS
[0027]
FIG. 1A is a perspective view of the collector.
FIG. IB is a perspective view of the example of FIG. 1A, applied to the skin of a
subject.
FIG. 1C is a further perspective view of the example of FIG. 1A, wherein the reservoir
is being removed.
FIG. ID is an exploded perspective view of one example of the collector showing the
base, actuator and lumen.
FIG. IE is perspective schematic of a micro fluidic channel of the collector comprising
two regions, a capillary-dominant region and a gravity- dominant region.
FIG. IF depicts the example of FIG. ID, wherein the fluid is in the gravity- dominant
region.
FIG. 1G is the distance traveled by fluid in channels of specific characteristics.
FIG. 1H is the distance traveled by fluid in a variety of channel designs.
FIG. 2A depicts a top-down cross-sectional view of the collector, according to one
example.
FIG. 2B depicts a top-down cross-sectional view of the collector, according to an
example.
FIG. 2C depicts a side view of the collector, according to an example.
FIG. 2D is a side view of the collector of FIG. 2C from an alternate angle.
FIG. 2E is a side view of a collector having multiple reservoirs, according to an
example
FIG. 2F is a side view of the collector of FIG. 2E from an alternate angle.
FIG. 3A is a top-down cross-sectional view of the collector, according to one example.
FIG. 3B is a side view of the collector of FIG. 3A.
FIG. 3C is a side view of the collector of FIG. 3A from an alternate angle.
FIG. 3D is a side view of a reservoir and outflow channel depicting a fluidic bridge,
according to an example.
FIG. 4A depicts a top-down cross-sectional view of the collector, according to one
example.
FIG. 4B depicts a top-down cross-sectional view of the collector, according to an
example.
FIG. 4C depicts a top-down cross-sectional view of the collector, according to an
example.
FIG. 4D depicts a top-down cross-sectional view of the collector, according to an
example.
FIG. 5A is a perspective view of the collector, according to an example.
FIG. 5B depicts a top-down cross-sectional view of the collector of FIG. 5A, showing
fitting and reservoir connection.
FIG. 5C depicts a top-down cross-sectional view of the collector of FIG. 5A, showing
fitting and reservoir connection, wherein the reservoir is removed.
FIG. 5D is a cutaway perspective view of the collector, according to an example.
FIG. 5E is a cross-sectional side view of the outflow channel and reservoir, according
to an examplet.
FIG. 6A is a detailed perspective cross-sectional view of an outflow channel and reservoir,
according to an example.
FIG. 6B is a perspective view of an open microfluidic channel which satisfies the
SCF relationship and can serve as a ramp in certain examples.
FIG. 6C is a perspective view of the channel of FIG. 6B, further comprising fluid.
FIG. 7A is a cross-sectional view of a surface tension valve in a closed position,
according to an example.
FIG. 7B is a cross-sectional view of the valve of 7A in an open position.
FIG. 7C is a cross-sectional view of an alternative example of a valve and channel
configuration in the collector.
FIG. 7D is a cross-sectional view of another alternative example of a valve and channel
configuration in the collector.
FIG. 8 is a further cross-sectional view of another alternative examplet of a surface
tension valve and channel configuration in the collector.
FIG. 9A is a cross-sectional side view of an example of an outflow channel in the
reservoir.
FIG. 9B depicts the channel and reservoir of 9A in a horizontal position.
FIG. 9C is a cross-sectional side view of an alternative example of an outflow channel
in the reservoir.
FIG. 9D depicts the channel and reservoir of 9C in a horizontal position.
FIG. 10 depicts a perspective cross-sectional view of a collection well, according
to an example.
FIG. 11 depicts a cross-sectional view of fluid flow through a channel having defects
according to an example.
FIG. 12A depicts a top view of one embodiment of microchannels comprising surface
tension guides, wherein gravity assists with the direction of flow.
FIG. 12B depicts a top view of the embodiment of FIG. 12A, wherein the fluid has progressed
through the microchannels.
FIG. 12C depicts another top view of an alternative example of microchannels comprising
surface tension guides, wherein gravity assists with the direction of flow.
FIG. 12D depicts a top view of the example of FIG. 12C, wherein the fluid has progressed
through the microchannels.
FIG. 12E depicts a side view of an example of a microchannel comprising at least one
rounded ridge.
FIG. 12F depicts a side view of an example of a microchannel comprising at least one
square ridge.
FIG. 12G depicts a side view of an example of a microchannel comprising the surface
tension guide is provided by a grooved, textured portion.
FIG. 12H depicts a side view of an example of a microchannel comprising a typical
open channel for comparison.
FIG. 13 depicts a cross-sectional view of a directional- flow branched channel, according
to one example.
FIG. 14A depicts a cross-sectional view of an example of the collector having an outflow
channel and two reservoirs.
FIG. 14B depicts the channel and reservoir system of 14A in a horizontal position,
such that fluid is directed into the second channel and reservoir by gravity.
FIG. 15A depicts a side view of a reservoir and outflow channel according to an example.
FIG. 15B depicts the example of FIG. 15A, wherein the fluid has been transferred to
the distal end of the reservoir.
FIG. 15C depicts the example of FIG. 15B in a horizontal orientation.
FIG. 16A depicts a perspective, transparent view of a reservoir and an example of
an outflow channel, wherein the channel is configured to be in direct fluidic communication
with the bottom inner surface of the reservoir when the collector is in a horizontal
position.
FIG. 16B depicts a perspective, transparent view of a reservoir and an exemplary example
of an outflow channel, wherein the channel is configured to be in direct fluidic communication
with the top inner surface of the reservoir when the collector is in a horizontal
position.
FIG. 16C depicts a perspective, transparent view of a reservoir and an example of
an outflow channel, wherein the channel is in a bulb configuration.
FIG. 16D depicts a perspective, transparent view of a reservoir and an example of
an outflow channel, wherein the channel is in a splayed configuration.
FIG. 16E is a perspective, transparent view of a reservoir and an example of an outflow
channel, wherein the channel is in a straight channel configuration.
FIG. 17A is a perspective cross-sectional view of a specific volume reservoir, according
to an alternative example.
FIG. 17B. is an end-view of the example of FIG. 17A.
FIG. 18A is a perspective view of a cartridge reservoir, according to an example.
FIG. 18B is a perspective view of an alternative example of the cartridge.
FIG. 18C is a reverse perspective view of further example of the cartridge.
DETAILED DESCRIPTION
[0028] The various embodiments disclosed or contemplated herein relate to a single device
that can be used by untrained or minimally-trained persons to both collect bodily
fluid and seamlessly contain the bodily fluid, and related systems and methods.
[0029] The present disclosure describes the use of microfluidic methods that utilize gravity
within open microfluidic channels in a manner which complements the capillary driven
flow, and enables new applications that were previously difficult to achieve, including,
but not limited to, adding a detachable tube, incorporating one-way flow valves, including
geometries more amenable to manufacturing methods, and using engineered connection
methods..
[0030] It is understood that the various embodiments of the devices and related methods
and systems disclosed herein can be incorporated into or used with any other known
medical devices, systems, and methods. For example, the various embodiments disclosed
herein may be incorporated into or used with any of the medical devices and systems
disclosed in co-pending U.S. Application No.
13/949,108, filed July 23, 2013, entitled "Methods, Systems, and Devices Relating to Open Microfluidic Channels,"
and U.S. Application No.
13/750,526, filed January 25, 2013, entitled "Handheld Device for Drawing, Collecting, and Analyzing Bodily Fluid,".
[0031] Disclosed herein are various embodiments of an integrated collection and containment
device that collects and transfers the bodily fluid from a subject's tissue into an
easily detachable tube or reservoir. Previous technologies approached the transfer
of the bodily fluid in a linear manner: one device enabled the bodily fluid to exit
the tissue and another device was used to collect the bodily fluid. In contrast, the
implementations disclosed herein simplify the process of bodily fluid collection by
integrating the collection of the bodily fluid directly with the containment of bodily
fluid within the same device.
[0032] Certain embodiments utilize gravity as a passive energy source to overcome surface
tension in specific and defined areas so as to facilitate the transfer of fluids.
As will become apparent, examples described herein include various apparatuses, systems
and methods for collecting fluid samples, such as bodily fluids, and enabling the
containment of those samples in containers that are easily attached and removed from
a collection device. Exemplary embodiments are for use in medical devices, at-home
diagnostic devices, and laboratory analysis platforms and equipment.
[0033] The ability to specifically and intentionally use gravity to overcome or enhance
capillary force is useful for the manufacturability of microfluidic channels. When
utilizing gravitational force in the direction of the fluid flow, the gravitational
force acts as an extra, or additive force to promote the flow of fluid in places that
have an unfavorable capillary drawing force for a variety of reasons. For example,
materials that have a high surface energy (and thus a large contact angle) often have
difficulty drawing fluid. If the channel is oriented such that the input is above
the output, fluid will naturally be forced through the channel due to gravity, overcoming
the unfavorable surface properties of the plastic and thus enabling a wider range
of plastics that can be used in a gravity-assisted capillary device. In certain implementations,
this benefit can extend to overcoming various manufacturing defects, allowing these
fluid systems to be particularly robust and easy to manufacture, as less precision
may be required. Manufacturing defects can include small surface or dimensional imperfections
that can create fluidic pinning ridges that would otherwise stop fluid flow, improper
manufacturing depth that would reduce spontaneous capillary flow, rounded channel
corners, dirt or dust particulates that may land in the channel during assembly, and
other imperfections that may exist in the channel and hinder fluid progression in
an entirely capillary driven device.
[0034] The creation or production of small, narrow channels via injection molding reveals
a difficulty in the fabrication of previous microfluidic devices. The aspect ratio
of height-width is an important parameter for successfully injection molding micro
channels. Microfluidic engineers generally prefer tall and thin channels for fluidic
functionality, whereas manufacturing engineers generally prefer short and wide channels
for ease of manufacturability. When utilizing gravitational force in the direction
of fluid flow, a microfluidic engineer can design channels that are shorter and wider
to accomplish the fluidic functionality needed for a system, in this case the transfer
of bodily fluids. Thus, the utilization of gravity enables complex microfluidic fluid
flow in microchannels that are easy to manufacture.
[0035] The various exampless described herein also include valves and channels that further
extend the functionality of the open microfluidic platforms being utilized. These
valves allow for more complex fluid handling within passive microchannels. For instance,
the valves can induce timed fluid release or specific volume releases using the disclosed
examples. Utilizing these same gravity enhancements with channels oriented in the
direction of gravity, channels can be designed to create a droplet, and have the droplet
connect to another channel after growing to a specific size. This droplet formation
can also allow the connection of the channel to any receptacle, including, but not
limited to, centrifuge tubes and other attached reservoirs. The step of creating a
droplet further allows specific boluses of fluid to be delivered, as the distance
to the channel or surface properties of the plastic change the size of the drop necessary
to allow gravity to dominate over surface tension and allow fluid flow. Because the
fluid is creating a droplet and falling into the next chamber, that chamber can then
be easily removed from the channel for further use. The ability to utilize capillary
and gravitational forces together to create efficient channels can result in devices
that are simpler, less expensive, and easier to manufacture and more robust in their
operation because they have higher working tolerances, therefore not requiring as
much precision in the channels. This can result in reduced unit cost. As these channels
can overcome larger differences in surface energy than capillary- driven devices,
the connections can be more easily made with a variety of less-specialized devices,
as in the cases of plastic centrifuge tubes or rubber septum reservoirs. The connection
with these parts can be easily severed to allow these parts to be removed from the
device and sealed with minimal secondary processes, enabling a bodily fluid reservoir
to either be connected with no backflow or disconnected from the device entirely or
some combination of those steps.
[0036] Finally, flow in capillary networks can be improved by utilizing gravitational forces.
Flow in capillary networks can be limited by two factors: the length of the network
and the vertical changes in height between areas of the network. As to network length,
increases in length result in corresponding decreases in capillary flow rate, due
to the resistance to flow developed by the wetted sections of the channel. The reduction
in flow rates is particularly difficult for viscous fluids or non-Newtonian fluids
which could render the network unusable. By designing a network in a three-dimensional
space that flows with the gravitational field, it is possible to counteract the resistance
to flow in order to accelerate or maintain at a constant velocity the flow of the
fluid in the network.
[0037] In the case of capillary networks that have differences in vertical height along
the length of the device, the weight of the fluid can cancel the capillary pull force
and prevent the flow from occurring. In these instances, there will be a point along
the length of the channel at which the fluid front, or leading edge, stops advancing
through the channel and which is dependent on the capillary number of the channel,
the geometry of the channel, and the composition of the fluid.
[0038] Turning to the figures with greater detail, FIGS. 1A-1F and 2A-F depict examples
of the gravity-enhanced fluid collection device, or simply "collector" 100. As is
shown in FIGS. 1A-B, in an example, the collector 100 generally comprises a housing
10 having first 12 and second 14 ends, and which is configured to be in fluidic communication
with at least one reservoir 104, such as a tube or cartridge by way of a fitting or
coupling portion 103, which is also called a "collar" in certain examples, and an
outflow channel 112. In exemplary embodiments, the reservoir 104 can be removably
attached to the housing 10, by way of the coupling portion 103, such that it maybe
detached, as is shown in FIG. 1C. In certain examples, the reservoir 104 can be a
standard Eppendorf tube press-fitted on the fitting 103. In further exampless, the
reservoir 104 can also be custom made and utilize capillary forces or solely gravitational
forces to fill. The tube 104 can thus act as a removable and standardized reservoir
104 for containing or gathering the fluid that can be simply and easily detached and
inserted into existing and established testing or lab equipment. By way of example,
where the fluid is blood, the tube 104 can be easily inserted into clinical and laboratory
equipment or workflows for diagnostics and/or biomarker detections.
[0039] In use, as best shown in FIG. IB, the collector 100 is placed on the skin of a user
such that the distal portion 104B of the fluid reservoir 104 is oriented in a substantially
vertically down position. As a result of this orientation, bodily fluids collected
at the collection sites 101 are drawn in by the fluidic network 102 for transport
out the fluid reservoir 104. In these examples, as best shown in FIG. 2A, capillary
forces allow the fluid to interact and be guided by the individual micro fluidic channels
102A, 102B, 102C of the fluidic network 102 which are disposed within the housing
to maximize the advantages of the channel geometries, while gravity biases the flow
of fluids into and through the fluid network 102. Additional description of the fluidic
and physical connection of the reservoir 104 is set forth below in conjunction to
FIGS. 3A-C, 5A-6 and 15A-16E, for example.
[0040] As is shown in FIG. ID, in exemplary embodiments, the housing 10 further comprises
an internal lumen 22, as has also been previously described in U.S. Application No.
13/750,526, filed January 25, 2013, entitled "Handheld Device for Drawing, Collecting, and Analyzing Bodily Fluid,".
Further, certain devices have at least one actuator 110, and are configured to be
placed against the skin of a patient 1, as is shown in FIG. IB. Upon depressing or
otherwise operating the actuator 110, at least one lancet, needle or other skin puncture
device (such as the four needles 30 depicted in FIG. ID, which is discussed below)
is deployed, so as to pierce the subject's skin and cause blood or other bodily fluid
to pool near the collection areas (as shown in FIG. 4A-D), for uptake into the microfluidic
network.
[0041] FIG. ID is an exploded perspective view of an example of the collector 100, in accordance
with one implementation. In this example, the actuator 110 functions as a plunger
18 configured to be inserted into the lumen 22 at the proximal end 12 of the housing
10. This plunger contains a face 28 and a plurality of needles 30 or lancets. The
plurality of needles 30 is fixed to the face 28. A base 20 attaches to the distal
end 14 of the housing 10 and contains a plurality of apertures, or collection sites
101 that are in fluid communication with the lumen 22 and match with the number and
positions of the needles 30 on the plunger 18 such that the needles 30 extend through
the apertures 101.
[0042] The plurality of needles 30 may include needles having a gauge from 20 gauge to 40
gauge. In some examples not being part of the invention, the needles are from 29 gauge
to 40 gauge. In an alternative example, the plurality of needles 30 may include a
plurality of microneedles. In the example shown in FIG. 3, the plurality of collection
sites 101 on the base 20 illustratively includes four apertures that match with the
needles 30. In alternative examples, the plurality of collection sites 101 may include
from two to one hundred apertures. The plurality of needles 30 are aligned to be guided
to pass through the plurality of collection sites 32 when a user actuates the actuator
110, thereby deploying the needles 30.
[0043] In certain examples not being part of the invention, a spring 24 is provided, which
retracts the plunger 18 through the lumen 22 from the distal end 14 to the proximal
end 12 of the housing 10 after the plunger 18 has been depressed and the force used
to depress the plunger 18 has been removed, thereby removing the plurality of needles
30 from the subject's skin and creating a vacuum in the vacuum creation space 22,
which is the portion of the lumen 22 distal to the plunger 18. In these examples,
the vacuum created in the lumen 22 creates a vacuum at each of the collection sites
101, thereby enhancing the pooling of bodily fluid on the subject's skin, optimizing
fluid extraction from each puncture site where one of the plurality of needles 30
penetrates the subject's skin, and at the same time minimizing the size of each puncture
site. The vacuum created may range from greater than 0 Pa to 75,000 Pa.
[0044] Within the various collector examples, a network of micro fluidic channels are utilized
to shuttle fluid from the various fluid collection sites to the outflow channel. As
will be shown with reference to FIGS. 1E-F, designing open or closed channels in a
collector that utilize a combination of capillary and gravity forces can be accomplished
by changing the geometry of the channel or properties of the fluids and device materials.
A characteristic number that can be used to design these channels is the Bond number,
which is Equation 1 :
where Δρ is the difference in fluidic density between the fluid flowing in the channel
and the fluid surrounding it, g is the gravitational constant, L is the characteristic
length of the channel, typically its width, and σ is the surface tension of the fluid.
[0045] For Bond numbers lower than 0.1, capillary forces serve as the primary driving forces,
and gravity is of lesser influence. At Bond numbers above 10, gravity becomes the
primary driving force. For Bond numbers between 0.1 and 10, both capillary and gravitational
forces have a definitive effect - that can compete, amplify, or alter one another.
For example, if a channel has a negative slope, gravitational forces will amplify
the flow and allow the flow to cross defects on the surfaces, grooves, and pinning
regions. On the contrary, if the channel has a positive slope gravity will reduce
the flow and potentially stabilize the effect of some surface tension features such
as pinning valves. Finally, capillary and gravitational forces can be used in conjunction
in the design of channels, as described herein, so as to enhance and otherwise direct
the flow of a collected fluid. For example, to drive a specific branch of a dividing
channel or flow around features that would be in the way of direct gravitational flow
by use of capillary features that direct the flow, as is discussed herein. Further,
the combination of gravitational and capillary forces can be used to create efficient,
cost-effective devices, systems and methods, like those disclosed herein.
[0046] These features are exemplified in FIGS. 1E-F, in which a channel 150 contains at
least two distinct regions. A first, more narrow region of high capillary force 151
(a low Bond number) and a second, wider region 1 2 where the Bond number is higher,
and gravity plays a more substantial role in the fluid flow. Fluid 154 will be readily
drawn into the first region 151 due to the high capillary force. Once the fluid reaches
the second region 1 2, given the high Bond number, capillary force is insufficient
to drive the flow alone, and gravity is then utilized to cause the flow to continue.
To function properly, the channel 150 has to have a negative slope relative to the
horizontal 153. Additionally, because less capillary force is being applied, these
channels can be designed to retain less fluid. As is described herein, the use of
these combinations of forces allows the collector's microfluidic network to achieve
fluid flow in a variety of applications.
Example 1 : Average Blood Travel Distance
[0047] FIG. 1G depicts the average blood travel distance for various channels under experimental
conditions. To test the travelled distance of fluid in channels with various geometries,
ports, and treatments, a channel of 700um x 1200um was tested with various channel
designs to assess the overall travel distance of the fluid. In this figure, * represents
p < 0.0001. with an n = 10 per condition. Error bars represent standard deviation
of the mean. In this example, the channels were designed with an aspect ratio of 700um
wide x 1200um, and the channels treated with 50% dextrose and 1.8mg/mL EDTA resulted
in optimal capillary draw. In FIG. 1H, the data for various channel geometries is
shown.
[0048] FIGS. 2A-B, depict top-down, cross-sectional views of the internal components of
two examples of a collector 100. In these examples, networks of microfluidic channels
102 utilizing both capillary forces and gravity forces can be used to shuttle the
blood down small scale channels (typically defined by a capillary number of less than
0.1) and larger channels respectively. In such small channels, the capillary forces
are the primary driving forces of fluid movement.
[0049] In such examples, and as best shown in FIGS. 2A-2B, the collector 100 comprises at
least one collection site 101A, 101B, 101C, 101D disposed within the housing 10, a
fluidic channel network 102, such as a microfluidic channel network 102, a coupling
portion 103, an outflow channel 112 and at least one reservoir 104. Various implementations
will feature a variety of numbers and configurations of collection sites, such as
the three sites 101 A, 101B, 101C shown in FIG. 2A or four sites 101A, 101B, 101C,
101D shown in FIG. 2B. Other configurations are possible. In various examples, as
best shown in FIG. 2A, the reservoir 104 further comprises proximal 104 A and distal
104B ends.
[0050] Certain embodiments further comprise at least one ramp 105, the microfluidic channel
geometry which can be defined so as to exploit the maximum vertical height attainable,
thereby facilitating the constant flow of fluids through various changes in height.
Specific channel geometries can be designed to facilitate fluid flow by the combination
of capillary and gravitational forces.
[0051] A more detailed explanation of the configurations and benefits of such ramps 105
follows. As open microfluidic channels contain open liquid-air interfaces, spontaneous
capillary flow can be utilized in certain settings to drive fluid flow. The use of
capillary-driven flow to manipulate fluids in complex open microfluidic networks is
a novel feature previously unused in open microfluidic channels. In order to insure
that spontaneous capillary flow ("SCF") occur in a channel containing any number of
open liquid-air interfaces in its cross-section, an analysis of capillary force to
define a design guideline ensuring that the capillary force provided by the walls
of the microfluidic channel overcomes the resistance created by the open sections
of the microfluidic channel.
[0052] The result of the analysis is written in a SCF relation stating that the ratio of
the free perimeter (pf), defined by the length of the cross-section open to air or
another medium, and the wetted perimeter (pw), defined by the length of the cross-section
made up of solid hydrophilic material must be less than the cosine of the contact
angle (Θ) of the fluid with the channel walls. The SCF relation can be written as:
[0053] Equation (2) thus defines the set of open channel geometries under which the SCF
relation is met. When the SCF relation is satisfied, the channel will drive the flow
through the microfluidic network by capillary forces, including against the force
of gravity. Importantly, the SCF relation extends to most channel configurations containing
open liquid-air and wetted sections. Further, the open liquid-air sections do not
have to be continuous or contiguous. Thus the SCF relation still holds for complex
channel geometries containing open "windows" on the channel (e.g. a circular aperture
in the wall of a channel) as well channels containing multiple open liquid-air interfaces
at the same point in the channel (e.g. a fluid completely suspended between two rails
in a channel devoid of ceiling and floor). Open microfluidic channels verifying the
SCF relation also have the benefit of not being constrained to rectangular cross-sections.
FIGS. 6B-C depict further views of these applications.
[0054] With that background in mind, a ramp (such as ramp 105) can be used to exploit the
maximum vertical height attainable. The vertical height change that a fluid can reach
can be evaluated experimentally and analytically using an equation relating to the
force of gravitational resistance (F = pg h) and the estimation of the force of capillary
pull (F = 2ycos (6*)/RF, where Θ<*>is the equivalent contact angle of the fluid in
an open microfluidic channel, and RFis the fluidic radius of the channel. Θ* is defined
as cos (0<*>) =∑ icos (0£), where represent the relative length of a section of the
channel wall that has a contact angle RFrepresents the fluidic radius of the channel
and is defined as RF= 2A/P, where A is the cross-sectional area of the channel and
P the perimeter of the channel). These two forces allow the estimation of the maximum
vertical height attainable by the fluid, as given in Equation 3
[0055] By way of example, in the case of the a rectangular channel of 1 mm width, 1 mm depth
and open on the ceiling, with a contact angle of 60 degrees on the plastic surfaces
and assumed to be 90 degrees in the open interface areas, filled with water, the maximum
vertical height attainable is evaluated to be about 10.5 mm. Further data can be seen
in Table 1.
[0056] As shown in Table 1, various channel geometries can be contemplated for a given material
contact angle (here assumed to be 60 degrees) that contemplate the theoretical maximum
vertical height attainable by the fluid, as given in Equation 3. Due to open channel
geometry, increases to the width of the channel will affect fluid travel against gravity
more than increases to the height. Table 1 depicts the net vertical height (in millimeter)
a fluid can travel against gravity. While the distance traveled may vary depending
on the orientation of the channel relative to the direction of gravity, the total
height achieved will remain the same. The calculated values are the theoretical total
height a fluid can travel directly against gravity, thus, as a channel is placed at
an angle not directly against gravity, the fluid will be able to travel a greater
length along the channel that will not exceed the total theoretical height. In practice,
one trained in the art can utilize the theoretical maximum height traveled to engineer
fluidic microsystems that contemplate the combination of capillary and gravitational
forces.
[0057] These numbers are well correlated with experimental data collected on such channels.
However, regardless of the geometry of the channel, a point of maximum vertical height
that a fluid can reach will always exist. The maximum vertical height attainable can
increase as the channel is held in various angles that are less than directly opposite
to gravity.
[0058] Utilizing the knowledge of the maximum vertical height for various channel geometries,
the disclosed collector examples can comprise microfluidic networks with channels
designed to facilitate the collection and movement of fluids by a combination of capillary
and gravitational forces in a variety of implementations. Additionally, the contact
angle can be modified by different treatments of the surface through plasma, chemical,
or physical additives. Additives to the channel to improve capillary drive can include
EDTA, heparin, dextrose, and other additives that when dried pull fluid up and into
the channel. The percentage of dextrose tested showed improved blood pulling capabilities
with 50% dextrose dried into the channel.
[0059] When utilizing gravity to direct fluid flow, more unique channel geometries can be
utilized. Therefore filling standardized reservoirs, such as centrifuge tubes or rubber
septum reservoirs is easily accomplished. Fluid can also be made to fill larger reservoirs
which typically have a low capillary number and thus more sensitive to gravity. Enhancing
the flow of blood using gravity also ensures reliability in fluidic connections, at
the specific location for example when the fluid must be transferred from the collection
device to a detachable reservoir. Typically the small gap that exists at these connection
points can act as barriers blocking the advancement of the fluid. With the addition
of gravity and well-designed channel geometries these gaps can be cleared reliably.
Thus, there is no need to engineer and manufacture specialized outflow channels and/or
reservoirs that have a short channel length in order to satisfy the fluid flow requirements
imposed by a gravitationally independent micro fluidic system. As is shown further
in FIGS. 3A- 3C and FIG. 6, these ramps can assist with the movement of fluid from
a collection site up and out to the outflow channel.
[0060] Returning to FIG. 2A, by utilizing gravitational force as a means of shuttling the
fluid, various examples can ensure that blood flowing down one of the branches 102
A, 102B, 102C of the micro fluidic network 102 do not substantially enter the other
branches, because, in use, the branches 102A, 102B, 102C are configured to be oriented
from the collection sites 101 to the coupling region 103 such that the direction of
flow is substantially in line with the direction of gravity (designated with the reference
arrow G). By way of example, in certain implementations, the flow can occur between
-60 and +60 degrees from the direction of gravity when rotated about the z (normal
to the bottom surface) axis. When rotated about the y (along the face of the bottom
surface, perpendicular to the direction of gravity in this case) axis, a rotation
comprised between +90 and -45 degrees was observed to be functional (FIG. 1A also
depicts the axis for reference). However, examples can be contemplated wherein any
direction vector that has a positive component in the direction of gravity will enable
flow.
[0061] In various examples, the flow will be proportional to the angle made by the microfluidic
channel relative to the direction of the gravitational force. In this manner, the
gravity-enhanced microfluidic networks are able to minimize the volume of sample lost
passively through backwashing or other non-productive flows in the channels. Further,
utilizing gravity-enhanced micro channels, it is possible to empty the channels at
the end of the fluid collection and further reduce lost volumes of fluid that may
remain within the fluidic network. In these examples, once the source of fluid - such
as blood flowing from a lancet puncture on the skin - stops providing additional fluid,
the channel will simply drain into the tube connected to the channel network. This
effect can be maximized by designing a channel that expands as it reaches the reservoir
so that capillary action becomes weaker as the fluid reaches the reservoir. Using
this approach, gravity will become the primary force, gradually overcoming the capillary
forces and thereby minimizing the amount of fluid remaining in the microfluidic channel
following outflow.
[0062] As shown in FIG. 2B, in alternate embodiments, the microfluidic network can be connected
to two or more tubes or reservoirs 104, 108. In this specific example, the reservoirs
104, 108 are positioned on alternate sides of the collector 100. Utilizing this approach,
the device 100 can allow the collection of fluid in one of the reservoirs 104, 108
even in the event that the user places the device 100 in the wrong direction. The
device 100 is similarly placed on the skin of the user in any vertical direction.
The bodily fluid pooling at the surface of the skin in the collection sites 101 is
captured by the fluidic channel network and, depending on the orientation of the device
100, gravity will bias its flow down the most descending channel. In one embodiment,
there are two channels 102 and 106, or alternatively there can be any number of channels
if more degrees of freedom on the placement of the device 100 are desired. As the
fluid flows through the channel (102 or 106), it will be raised from the plane of
the channel network into the reservoirs by fluidic ramps 105 or 107, as is described
further below in relation to FIGS. 3A-C and 5A-6. Reservoirs 104 and 108 are connected
on each end and the reservoir (104 or 108) located lower vertically will become the
reservoir receiving the fluid. In other examples, any number of reservoirs can be
designed. In yet other examples not being part of the invention, these reservoirs
can be standardized Eppendorf tubes press fitted onto the device 100 by a fitting
103. Importantly, as the fluid does not enter or minimally enters channels that go
in an ascending direction, the addition of these channels does not incur a loss of
fluid. Further, in certain examples in which the capillary number is low, the fluid
will be drained from the channels into the reservoirs at the end of the fluid collection
or fluid flow, minimizing the loss of fluid in the reservoirs. FIGS. 2C-F depict various
exterior side views of the examples of FIGS. 2A & 2B, including the various shapes
of the actuator 110 and the orientation of one or more tubes or reservoirs 104, 108.
[0063] As shown in FIG. 3A-C, in certain examples, the collector 200 is configured such
that fluid is collected in a detachable tube or reservoir (as shown in FIG. 1C, for
example) or standardized tube using a U-shaped, suspended, or outflow channel 205
that extends into the center of the tube (such as tube 104 of FIGS. 1A-C) as part
of a tube connection 206 and can be elevated from the initial collection site by a
channel 207 which serves as a ramp 207 (as best shown in FIGS. 3B-C). By using open
microfluidic system ramps 207 for fluids, the various embodiments of the collector
200 can be configured so as to raise or lower the channel plane to any level (as can
be seen, for example, in reference to 422 in FIG. 6), such that the relative height
of the fluid flow can be changed without reducing or stopping the fluid flow. These
movements of fluid in a vertical direction (up or down) can also contribute to the
enhancement of the fluid flow. Accordingly, the fluid can be directed through the
outflow channel 205 and into a reservoir or tube (such as tube 104 of FIGS. 1A-1C).
[0064] In operation, the collector 200 is placed on the skin of the user (such as shown
in FIG. IB with respect to another collector example). As described, blood being collected
at one or multiple collection sites 201A, 201B, 201C are captured in a fluidic channel
network 202, which comprises a plurality of branched channels 202A, 202B, 202C which
are disposed so as to utilize both capillary and gravitational forces when the outflow
channel is oriented in the direction of gravity G. When the fluidic channel network
is placed in a descending manner, gravity will enhance the flow of fluids down the
channels 202A, 202B, 202C. As discussed above, in certain embodiments, a ramp 207
can be used to connect the fluids flowing in the network to the outflow channel 205,
which allows the filling of a reservoir (not shown). As with the example shown in
FIG. 1C, the reservoir (not shown) used with the connector 200 can be a detachable
reservoir that can be removably connected to the device 200. In the example of a standard
test tube, the fitting can be a simple press fitting region 204 to which a standard
tube is reversibly coupled to create a fluidic seal. In examples, these fittings may
be twist or snap fittings, as would be apparent to one of skill in the art. The fitting
206 is sealed to the reservoir, such that the connecting fluidic channel or outflow
channel 205 spans into the reservoir (as shown in FIG. 6), thereby allowing the fluid
flowing into it to touch a wall or other feature of the reservoir. This serves as
a fluidic bridge (which is also called a "capillary bridge") which allows the fluid
to transfer into the reservoir, as is described for example in relation to FIGS. 9A-D
and 15A-16E.
[0065] The collector 200 is thus able to collect fluid from a site on the subject's skin
and shuttle it to the outflow channel 205 using a combination of capillary and gravitational
forces. Once the fluid reaches the distal outflow channel 205, it is preferable to
have it flow into the reservoir (not shown) as efficiently as possible. As is shown
variously in the figures, in certain examples the outflow channel can extend the length
of the tube/reservoir such that the flowing fluid is able to contact the internal
distal end of the tube or reservoir (as is shown in FIGS. 9A-D at 905 and discussed
below). In further examples, the outflow channel extends partially into the tube,
thereby allowing the collected fluid to contact a side of the tube and descend to
the distal end (as is described further below in relation to FIGS. 15A-16E). Accordingly,
the outflow channel can be placed at any height relative to a longitudinal plane of
the tube or reservoir, thereby allowing the contact of the fluid at any location in
the tube, as is desired by the user based on the specific application. Further, gravity
can be used to enhance the ability of fluids flowing down the outflow channel to interact
and contact the reservoir or tube). In certain examples, an extended microfluidic
outflow channel allows for a preferable connection with a wall or floor of the reservoir
or tube by creating a simple fluidic bridge which allows reliable flow of fluid into
the reservoir. In these examples, gravity can be used to simply induce a positive
curvature of the fluid in the outflow channel such that the fluid bridges to the reservoir
and can contact a feature even in the presence of an air gap between the outflow channel
and the wall of the reservoir. Gravity can thus also be utilized to create a drop
of fluid that will only contact the walls of the reservoir of the tube when a sufficient
volume drop has been reached. Further examples are described in relation to FIGS.
9A-D and 16A-E.
[0066] As is shown, for example, in FIG. 3D, in certain examples a fluidic bridge 209 is
established between the outflow channel 205 and the reservoir 208, thereby forming
a fluidic bridge 209 and enabling a continuous flow of the fluid 210 into the reservoir
along the inner wall 208A of the reservoir 208. Further, this embodiment can be utilized
as a conditional valve for preventing the reverse flow out of the reservoir once the
fluid has been collected and the device is placed in a different orientation, as is
shown in FIGS. 9A-9D. When placed in an orientation where the reservoir or tube is
located at the lowest point, the fluid flows into the reservoir and fills it. After
the flow has stopped and the device is placed on a horizontal surface, such as a laboratory
benchtop or a desk, the fluid may move to fill the tube sideways. Provided less than
a determined volume of fluid was collected in the tube, the level of the fluid will
not reach the channel in this orientation and thus prevent any backflow into the device.
Further examples are described in FIGS. 15A-C, 16A-E.
[0067] FIGS. 4A-D depict further examples of the collector 300, wherein the microfluidic
channel networks 302 are configured to utilize both capillarity and gravity to perform
essential fluidic functions. In these examples, the collector 300 is configured to
collect fluids from the various collection areas 301A, 301B, 301C, 301D and to shuttle
the fluid through one or more microfluidic channels 302A, 302B, 302C, 302E, 302F,
302G, 302H to a connection 303A, 303B to a reservoir or analytical device (not shown).
In these examples, at least one of the channels 302 A, 302B is placed in a descending
orientation (as described previously in relation to FIG. 2A), and multiple channels
302 can be used to increase the probability and/or ensure that at least one of the
channels 302 is in such a descending orientation.
[0068] As is shown in FIG. 4A, fluids collected in a large open area 304 or fluids flowing
down from another collection area 301 and reaching a large opening 304 can be guided
using a capillary ridge 305 in the direction of a channel 302. Capillary forces (in
the form of Concus- Finn effects for example) on a wedge and angle of the ridge or
ridges 305A, 305B will promote the liquid in the form of drops or a continuous flow
to remain close to the ridge, or ridges 305 A, 305B, as would be apparent to one of
skill in the art. In these examples, gravity will promote motion of the droplets or
slow continuous flow of fluid downwards until it reaches the opening of a channel
302A, 302B. In such examples, the ridge is configured to facilitate continuous fluid
flow due to the capillary forces created. In various similar examples, there is a
geometric shape or a sufficiently low surface energy introduced such that the shape
drives the capillary action whereby the capillary forces are a principle driving force
underlying fluid flow.
[0069] In the example of FIG. 4B, various inner channels 302C, 302D, 302E, 302G can connect
fluid from one or more fluid collection sites 301A, 301B, 301C, 301D such that fluid
from a first collection site 301 A will flow downstream through a channel 302G to
reach a second collection site 30 IB. Further, the fluid can be directed around the
collection site utilizing capillary forces and gravity by designing a wedge 307A that
links a first collection site 30 IB with the channel 302B opposite a second collection
site. These wedges 307A, 307B, 307C, 307D surround the fluid collection sites 301A,
301B, 301C, 301D and allows the fluid to link into the channel by wedge fluid flow.
In an example, the wedges are recessed plastic wedges around the collection sites
301A, 301B, 301C, 301D, which are therefore sent into the luminal side of the base
20 on the distal end 14 of the housing 10, as shown in FIG. ID and would be apparent
to one of skill in the art. Accordingly, provided that the fluidic path is consistently
and substantially in line with gravity, fluid inputted from each "higher" collection
site can be transferred around the lower collection site in a controlled, robust,
and clean way. This method prevents needless flow of a previously collected bodily
fluid over an exposed skin area for example.
[0070] In another example shown in FIG. 4C, fluid collected from each collection site 301
A, 301 B, 301C, 301D can be transferred through channels such as open micro fluidic
channels 31 OA, 310B, 3 IOC, 310D in which capillary force dominates into channels
302A, 302B, 302C that are biased by gravity. In this example, as the fluid in each
open micro fluidic channel 310 reaches gravity channel 302, it will flow in the descending
direction, or direction of lower potential energy, as described in relation to FIGS.
1E-F, for example. This system allows the minimization of the overall number of channels
required as all collection sites feed into a common channel that can be used bi-directionally.
[0071] In yet a further example, and as shown in FIG. 4D, the capillary channels 315A, 315B,
315C, 315D transferring bodily fluids from the collection sites 301A, 301B, 301C,
301D can be placed in any direction because they are dominated by capillary forces,
and once they reach a main channel 302A, 302B, gravity will bias their flow in the
descending direction toward the lower outflow channel 303A, 303B. This allows for
flexibility over where the fluid is delivered between the collection sites 301A, 301B,
301C, 301D and the main fluidic network 302A, 302B. Importantly, Concuss-Finn effects
in the wedges of the main channel can be utilized to promote the extraction of fluids
from the capillaries 315A, 315B, 315C, 315D. At the point of contact between the capillary
channels 315A, 315B, 315C, 315D and the main channels 302A, 302B the use of a rounded
junction and/or sufficiently low surface energy of the material will allow fluid to
robustly flow out of the capillary channels 315A, 315B, 315C, 315D, into the main
channels 302A, 302B, where the flow of the fluid will be enhanced by gravity.
[0072] The various examples depicted in FIGS. 5A-6 demonstrate a further integrated blood
collection and containment device, or collector 400. In various examples, the collector
400 features at least one closed-open or one open-closed-open microfluidic system
configured to promote the flow of fluid from the internal microfluidic channel network
(described in relation to FIGS 1A-4) into a detachable reservoir 402. One aspect is
a detachable reservoir 402 which is capable of being separated from the integrated
collection device 400 for seamless integration into existing laboratory processing
methods and processes, as it may be easily fitted to coupling region 408 and/or the
skirt 410 of the device 400 and later removed, as is shown in FIG. 5C at reference
arrow A. In these examples, the tube or reservoir 402 is coupled to the device 400
at the collar or plastic skirt 410 which creates a fluidic and/or air-tight seal with
the inner surface 401 of the reservoir 402. The inner surface 401 is correspondingly
in fluidic and physical communication with an outflow channel 414 contained within
an outflow channel housing 412 (as described at surface 420 in relation to FIG 6)
such that fluid collected by the device flows through the microfluidic channel network(s)
as a fluidic bridge into the reservoir 402 for collection by way of capillary and
gravitational forces. Further examples of the fluidic bridge and outflow channel are
discussed in relation to FIGS. 3D and 15A-16E.
[0073] In particular examples, the collector 400 functions by being placed on the skin of
the user or subject (similarly to the steps of the example described above and depicted
in FIGS. 1A-C) with the reservoir 402 directed downwards (relative to gravity) and
depressing the actuator 404. In various examples not being part of the invention,
the device 400 and reservoir 402 may comprise a hermetic or fluidic seal 401, and
the actuation of the button 404 may cause the pressure in the device 400 and reservoir
402 to decrease, thus enhancing the blood flow out of the skin of the user. Gravity
and capillary force then guide blood into the reservoir 402, as was previously described.
In certain phases, the driving force behind the fluid draw can be caused by microfluidics
and/or pressure differential. By way of example, in certain implementations the pressure
differential can be the primary force in drawing fluid out of the skin into the channels,
while the microfluidic forces account for the movement of blood through the channel
or network.
[0074] Specifically, being able to transfer the collected bodily fluid sample from an integrated
microfluidic collector 400 into a reservoir 402 or other collection reservoir that
is easily detachable from the device is novel in the field of capillary blood collection.
The bodily fluid collected from the patient is transferred through an outflow channel
414 into the reservoir 402. At the end of use or when the desired volume of blood
is collected in the reservoir 402, it can simply be detached by pulling it off by
several known methods, such as a press-fitting or twisting it off of a threaded structure
408A which is defined on the fitting 408.
[0075] The fluidic connection allowing robust transfer of the bodily fluid between the device
400 and the reservoir 402 is created through the outflow channel 414. The outflow
channel 414 is capable of being inserted into the tube, which is correspondingly sealed
around the plastic skirt 410. Accordingly, in examples, the micro fluidic outflow
channel 414 is comprised of the first open micro fluidic channel 424 in fluidic communication
with the internal microfluidic channel network described in relation to FIGS. 1A-4C.
In these examples, the first open microfluidic channel 424 functions as a ramp, as
described for example in relation to reference numbers 105 and 107 in FIG. 2.
[0076] This outflow channel 414 is detailed further in reference to FIG. 6. In certain examples,
the outflow channel 414 is further comprised of several microfluidic channels 424,
418, 422, and configured such that one of these microfluidic channels has a portion
422 facing the reservoir 402. Returning to FIGS. 5A-6, from this first "open" area
424, the fluid is then able to flow to the "closed" microfluidic channel 418, and
then again to a second "open" microfluidic channel 422, such that it is urged or otherwise
brought into contact with the inner surface 420 of the tube 402 and collected in the
reservoir 402 by way of a fluidic bridge. In these examples, the open microfluidic
system therefore allows capillary flow of the blood to the exposed portion, allowing
contact of the blood or bodily fluid with the reservoir 402.
[0077] Accordingly, and as shown in FIGS. 5D-6, the shape the outflow channel 414 can vary
along its length to first enhance capillary flow to include a closed microfluidic
channel 418 and progressively increase the cross-sectional length connected to the
inner surface of the tube 420 (as is shown at the ramp at 422) in order to force the
fluid to connect with the inner tube surface, bridge and flow into the reservoir 402.
Accordingly, open microfluidics associated with gravity allow the flow of blood along
an outflow channel 414 without causing it to "pin" or otherwise stop or pool when
the fluidic path suddenly opens into the reservoir 402. These open microfluidic methods
allow the gradual transition towards creating a drop of blood or a blood connection
with the tube, thereby preventing blocking, pinning, or clogging. As best shown in
FIG. 5E, the air opening 416 between the volume of air contained in the reservoir
402 and the volume of air in the device 400 with the shape of a cylinder or any other
shape allows the equilibration of air pressures between the reservoir 402 and the
inside of the device 400 while the fluid is filling the reservoir 402.
[0078] In various embodiments, certain open micro fluidic channels, such as those depicted
in FIGS. 6B-C. In embodiments wherein the ramps are working against gravity, they
may be composed of free surfaces and wetted surfaces satisfying the SCF relation (as
laid out by Eq. 3, stating that the ratio of the length of the cross-section of channel
spanning over the at-least one free surface the length of the cross-section of channel
spanning over the at-least one wetted is less than the cosine of the contact angle
of the fluid on the wetted surface), which thereby allows spontaneous capillary flow.
In various alternative examples not being part of the invention wherein the ramps
work with the assistance of gravity, the SCF relation need not be satisfied.
[0079] Importantly, the ability to connect an integrated blood collection device with a
detachable reservoir 402 or cartridge (shown in FIG. 19 at 1900) has many advantages.
One advantage is the ability to simply couple or otherwise interface the reservoir
with downstream equipment and measuring devices. The ability to simply press or screw
a tube or other collection device onto the integrated blood collection device allows
the use of any desired tube for downstream applications, including tubes for various
assays and applications, such as PC , which in certain examples may contain PCR reagents,
as shown at 426 in FIG. 6, as well as various microcentrifuge tubes, tubes containing
gel for plasma separation, standard tubes used in blood analysis laboratories for
pediatric applications, tubes that perform a specific assay directly within the tube,
tubes that stabilize or otherwise store the blood for shipping, and capillary blood
collection tubes. The tubes connected to the integrated bodily fluid collection device
can also be specific to blood collection, including tubes that contain EDTA, heparin,
serum separation gel, biomarker stabilization reagents, or any other pre-processing
blood collection tube. A tube can also be replaced by a customized reservoir that
is used for dedicated downstream equipment or processes. While the examples provided
herein refer to a tube, as would be apparent to one of skill in the art, various fluid
containers are well within the scope of the examples described herein.
[0080] Another advantage of the detachable reservoir being in fluidic communication with
the outflow channel is that the fluidic transfer from the tissue to the reservoir
is engineered to simplify the multi-step process of blood collection into a single
step process. Therefore, the user of the device does not need to be trained in the
art of tissue puncture, device handling during the fluid transfer process, or post-collection
processes including tissue sealing, handling of an exposed biospecimen, or other processes.
The integrated collection device described includes open microfluidic fluid transfer
but the device can perform the fluid transfer using any number of transfer mechanisms
including metal tubing, plastic tubing, and/or sealed microchannels. The tube or reservoir
is sealed from the exterior environment post-collection and can remain so during detachment
of the tube and after the tube is detached. The tube or collection reservoir filled
with the bodily fluid can be detached by twisting, pulling, activating a release mechanism,
or any other secondary step. This tube can then also have a known features, device,
or component that provides for self-sealing the tube during and following detachment.
Alternatively, the removal mechanism can activate other steps that may be helpful
in stabilization, sample preparation, or diagnostic analysis.
[0081] Gravity-enhanced microfluidics can be utilized to precisely control the nature of
the fiuidic connection between the device and the tube. In the example described in
FIGS. 5A-6, only a single section of the open microfluidic path 422 is removed to
allow connection with the tube 420, thereby ensuring that sufficient capillary force
allows the fluid to be flowed past the change in geometry, as is also described in
the commonly assigned
US Patent Application No. 13/949,108, filed on July 23, 2013. A central aspect to such embodiments is the ability to reliably transfer fluids
between a collection device and a reservoir utilizing open microfluidic systems.
[0082] The use of such open microfluidic methods allow for outflow channels 414 that can
be transiently in contact with a reservoir, container, or reservoir 402 while allowing
reliable and simple fluid transfer between the various aspects. In certain examples,
the outflow channel 414 favors capillary flow at the innermost aspect by presenting
a closed channel geometry thus allowing a robust draining of the fluid into the outflow
channel from the microfluidic network. Progressively, the geometry of the fiuidic
path along the outflow channel varies to an open channel configuration in which part
of the fluid is allowed to come in contact with the air or a different surface, as
is shown at 422. In order to ensure a strong probability of contact, that interface
must be large enough to allow the fluid to contact the new surface and create a drop
of sufficient volume that it flows by itself on the surface 420. This flow can be
enhanced by surface treatment of the reservoir through a surface activation or the
addition of a dried reagent that reduces the surface energy of the material and allows
increased wetting by the fluid or implementing a material in the manufacture of the
features that has a preferential surface energy, such as a hydrophilic plastic. Importantly
as there is no binding material between the outflow channel and the receptacle or
tube it can be removed or placed back in contact when needed.
[0083] As is shown in FIGS. 6B-6C, these open microfluidic channels 450 typically involve
at least one free surface 452 and at least one wetted surface 454 defining boundaries
of a cross section 456 known as the "free perimeter" (at 462) and "wetted perimeter,"
(at 454) respectively. In certain exemplary embodiments, the cross-section 456 of
the microfluidic channel 450 verifies the SCF relation stating that the ratio of the
length of the cross-section spanning over the at-least one free surface 452 to the
length of the cross-section spanning over the at-least one wetted surface 454 is less
than the cosine of the contact angle 458 of the fluid 460 on the wetted surface 454,
ensuring that fluid spontaneously flows by capillary force along the open channel
450.
[0084] FIGS. 7A-7D provide expanded views of microfluidic channels 800 such as those incorporated
into the various collector examples discussed above. As shown in FIGS. 7A-B, in various
embodiments of the gravity-enhanced microfluidic system 800, the flow of fluid 801
through a channel 802 can be regulated by way of a surface tension valve 805 placed
between the first 800A and second 800B channel portions or lengths and configured
such that the fluid 801 reaches a gap 807 in the channel which comprises the surface
tension valve 805 and is only able to span over the gap 807 by creating a drop-like
feature 803 able to flow along the channel 800. In examples, this is only possible
when the channel 800 is placed substantially vertically (as by rotation around reference
arrow A) such that the fluid is flowing with the gravitational field (shown by reference
arrow G). In these examples, an opening 807 is created in the channel path 800 between
the first 800A and second 800B channel lengths such that the fluidic network is disconnected
for most traditional fluid flows, as shown in FIG. 7A, where the surface tension valve
805 is preventing the flow of fluid 801 through the opening 807.
[0085] As is shown in FIG. 7B, when the channel 800 is oriented in a substantially vertical
position, the additional force of gravity allows the fluid 801 to overcome these surface
tension forces in the gap 807, thereby forcing the fluid to connect with the second
portion 800B of the fluidic channel. In these examples, once the fluid 801 contacts
the second channel portion, a sustainable fluid path is created allowing flow. Further,
when the channel 800 is returned to a substantially horizontal position, fluid is
then unable to flow back into the first portion 800A fluidic network.
[0086] As is shown in FIGS. 7C-D, in another example, fluid 801 flowing down a first channel
portion 800 reaches a gap 807 in the channel 802 and is only able to span over the
gap 807 by creating a drop-like feature 803 that contacts the second channel portion
800B, which in this example further features an expansion 810. Once the fluid 801
has connected to the second channel portion 800B, it is able to fill a reservoir 811,
which is situated opposite the expansion 810. At any time or at the end of the flow,
a lid 812 can be placed in the gap 807, allowing the sealing of the second half of
the micro fluidic channel 810 as well as the reservoir 811.
[0087] As is shown in FIG. 8, in an alternative example, a first channel portion 800A can
be designed to control delivery of fluid 801 into a second channel portion 800B. Fluid
801, flowing in a channel 800, again reaches a gap 807 in the fluidic network and
expands into a drop-like feature 803 if and only if the fluid is flowing in the direction
of the gravitational field, as has been discussed. Once the drop-like feature 803
connects to the second channel portion 800B, a pre-determined volume of the fluid
will be released from the drop-like feature 803. In these examples, the connection
occurs when a droplet (the volume of which is easily determined though standard equations)
reaches a height that is equal to the length of the gap 807. At that volume, fluidic
connection occurs, the droplet is drained to the other side, and the interface recedes
to a low volume position. The fluid 801 is thereby applied to the second channel portion
800B periodically and with controlled and tailored volumes. The addition of additional
channel features 804, such as capillary fins, surface tension guides, protrusions
or thin-walled ridges disposed within the second channel 800B can assist in the wicking
of the expanding drop-like feature 803 into the second half 800B of the micro fluidic
network. Once the drop-like feature 803 is released, the fluid in channel 802 will
recede back to the position of the gap and in reference to the Bond number discussed,
e.g., in relation to FIGS. 1E-F. In various implementations, this process can repeat
as long as there is available fluid 801 to be delivered to the system.
[0088] In the example depicted in FIGS. 9A-D, various microfluidic networks 900 can be utilized
which connect with a reservoir, or tube 904 (as discussed variously herein, such as
in relation to FIGS. 1A-C) such that fluid 906 can flow into the tube 904 when upright
(as is shown in FIGS. 9 A & 9C), but not flow back out of the tube 904 when placed
horizontally (as is shown in FIGS. 9B & 9D). This can be accomplished by designing
a channel with an appropriate Bond number relative to the angles at which it will
be disposed, as is discussed above in relation to FIGS. 1E-F. In these examples, gravity
is significant, and the fluidic paths will be influenced by gravity such that they
may take different paths as the device is placed in different orientations.
[0089] In these examples, when the collection device 901 is substantially upright (as depicted
in FIGS. 9 A and 9C), the fluid 906 is able to flow through the internal microfluidic
network 902 (as described in relation to FIGS. 2A-4D) and is raised from that channel
surface through a ramp 903 into the tube 904 by capillary action and gravity. An outflow
channel 905 is in fluidic contact with the inner surface of the tube 904 (which may
occur either at the top or bottom of the tube, as is also described in relation to
FIGS. 16A-B). The outflow channel 905 thereby delivers the fluid 906 into the tube
904 either by proximal fluidic connection with the bottom of the tube so as to create
a fluidic bridge and fill the tube (FIG. 9A) or by creating a fluidic bridge 907 with
the side of the tube (shown in FIG. 9C) that drips down the side and into the tube
904, thereby filling it.
[0090] When moved to the horizontal position (as depicted in FIGS. 9B and 9D), if the fluid
906 falls to the bottom of the tube 904 or if the fluid is capillary pinned in the
tube 904 via changes in surface tension, such as by changing the tube design, engineered
micro fluidics, material selection and/or low fluid volume, the fluid 906 cannot flow
back out of the tube 904 into the device 901. In this way, bodily fluid can be collected
and prepared for removal or shipping without the possibility of leakage.
[0091] An example depicted in FIG. 10, further comprise a reservoir 1000 which is a detection
well 1004. In these examples not being part of the invention, the well 1004 is configured
such that electronic probes having detection pads 1003 can be integrated into the
well 1004 by one or more electrical leads 1002 so that fluids can be applied to the
well 1004 by one or more outflow channels 1001. One of the obstacles to placing leads
into wells is that leads cannot be run across or over right angles, and instead require
less abrupt changes in direction for fabrication simplicity. In these examples, an
open well 1004 is provided such that at least one outflow channel 1001 can deliver
fluids into the open well 1004 and electrical leads 1002 can be integrated into the
well for analysis and detection by way of the pad 1003 or pads in a manner which does
not require the leads to be placed over a sharp corner.
[0092] The smooth transition 1006 enables electrical contact of the lead 1002 with the detection
pad 1003 during its transition into the well 1004. Utilizing gravity ensures the filling
of the open well 1004 as fluid is flowing down from outflow channel 1001 despite the
well 1004 not having a defined contour on its entire periphery 1005. The ability to
define smooth transitional surfaces 1006 into the well 1004 facilitates low-cost electronic
patterning technologies, including ink-jet printing. Further, in the depicted example,
the outflow channel comprises an outflow channel 1001 which is a deep channel 1001
which is further in fluidic communication with a connecting channel 1007, thereby
allowing the controllable flow of fluids through the connecting channel 1007 across
the smooth transition 1006 by the formation of a fluidic bridge, as has been previously
discussed. In various examples, these electric leads 1002 can be easily imprinted,
ink jet printed, or patterned into the well 1004 by a shallow and smooth transition
1006.
[0093] The use of gravity in combination with capillary forces allows the collector to overcome
manufacturing defects. By way of example, FIG. 11 depicts a channel 1101 that can
be incorporated into any of the collector examples discussed elsewhere herein, such
as in the micro fluidic network within the lumen, the outflow channels, or ramps.
This exemplary channel helps to explain some of the benefits of gravity-assisted micro
fluidic devices with respect to manufacturing due to the reduction in the need for
precision. When the channel 1101 is held in a position that allows the fluid flow
to be assisted by gravity, fluid 1102 can flow past pinning ridges 1103, which can
result from unintentional manufacturing defects, dust particles, or other capillary
interferences. This ability to pass such ridges 1103 to make the fluid flow, and therefore
the collector devices more reliable. Accordingly, in various examples, the precision
of the channel dimensions and/or configurations can be reduced while maintaining reliable
fluid flow.
[0094] As is shown in FIGS. 12A-D, by using gravitational assistance, certain exemplary
embodiments of the collector can comprise microchannels which contain surface tension
guides which can run substantially the length of the channel 1200 and influence the
direction of fluid flow within it. More specifically, in various embodiments, these
micro fluidic channels 1201 can be designed with surface tension guides 1202 in the
form of fluidic pinning ridges or hydrophilic patterns 1202 which allow a fluid 1203
to be guided in a specific direction. In this way, when the devices are oriented such
that gravity assists the direction of the flow (as is shown in FIGS. 12A-D), fluid
can be more specifically manipulated and moved for more complex fluid motion. These
manipulations can involve bends in the channel 1204, engineered fluid flow such as
velocity or other features that are known to those of skill in the art.
[0095] As shown in FIGS. 12E-H, the surface tension guides, ridges, or patterns, are simple
features that add texture or grooves in the surface, preferably with sharp edges that
will incur Concus-Finn capillary flow in the direction of the texture. As can be seen
in FIG. 12E, in one example, at least one rounded ridge 1210 can be provided within
the channel. As shown in FIG. 12F, at least one square ridge 1212 is given. In FIG.
12G, the surface tension guide is provided by a grooved, textured portion 1214, and
in FIG. 12H, a typical open channel 1216 is shown for comparison.
[0096] FIG. 13 depicts an alternative example comprising a bifurcated channel having a primary
channel 1302, first 1302B and second 1302C branches and, wherein the channel 1302
is configured to prohibit backflow into an unused branch (such as branch 1302C or
branch 1302B). In this example, the primary channel 1302 is oriented so as to have
a component of the gravitational force 1301 influence the fluid flow such that fluid
1304 from 1306 will be urged to flow to a confluence or junction 1305 and flow preferentially
in the direction of gravity 1301 and into the primary channel 1302 without flowing
up into the empty channel 1302B via capillary force. As would be apparent to one of
skill in the art, the use of a combination of gravitational forces to overcome any
capillary forces can be dictated by the specific application.
[0097] In the example of FIG. 14A-B, the collector can be used to deliver fluid in a timed
manner. In these examples not being part of the invention, fluid 1404 is collected
from a site 1401 and directed along a first channel 1402 into a reservoir 1403. In
these examples, collected fluid 1404 can then exit the reservoir 1403 when placed
horizontally (FIG. 14B) to flow back through the collection channel 1402, through
a second channel 1405 and into a second reservoir 1406, because of the introduction
of gravitational forces. In certain examples, this second reservoir 1406 can also
utilize gravitational assistance to allow fluid to flow exclusively into the second
channel 1405 instead of the first channel 1402. In this way, tests that need specific
timing of fluid addition for chemical reactions or other more specific biological
reactions can have the fluid enter the testing chamber (second reservoir 1406) as
a single bolus of fluid.
[0098] Microfluidic channels such as those discussed in relation to the outflow channels
tend to retain fluid. This creates two specific design issues. First is the desire
to collect as much fluid from the channel as possible in the reservoir. Second is
the need to prevent fluid backflow into the outflow channel when the orientation of
the reservoir is changed and fluid which has gathered in the reservoir can come back
into contact with fluid retained in the outflow channel, thus causing backflow. Various
outflow channel examples are disclosed herein which address aspects of these issues.
In certain implementations, the outflow channel is in direct fluidic communication
with the side of the tube, such as is shown in FIG. 3D. However, when inverted or
positioned such that the tube is on its side (or horizontal), these examples may allow
a simple fluid path for the fluid to drain back into the collector. To avoid this
reverse fluid flow, various alternative outflow channel geometries were created that
will allow device inversion without contact between the fluid and the outflow channel,
such as those discussed at FIGS. 9A-D and in relation to FIGS 15A-16E.
[0099] FIGS. 15A-D depict various examples of an outflow channel 1500 that allow device
inversion without the fluid in the tube coming into contact with the outflow channel
and the fluid retained there, as shown in FIG. 15B. In these examples, the outflow
channel 1500 extends from the collector such that the distal end of the channel 1500is
disposed within the tube or reservoir 1502, thereby providing the initial transitional
point for the flow of fluid 1 04 (as is described herein, for example, in relation
to FIGS. 5A-6C). The outflow channels in FIGS 15A- D and 16A-E are similar in that
they contemplate outflow channel geometries that act as oneway flow valves. In this
sense, the fluid is able to flow by dripping into the tube, but when the device and
tube are inverted, the channel 1500 will not allow backflow out of the tube.
[0100] This specific action is shown in FIGS. 15A-C. In FIG. 15A, the fluid 1504 flows out
of the outflow channel 1500 into the tube 1502. When the flow of fluid 1504 is complete
as shown in FIG. 15B, the fluid 1504 is within the tube 1502. When the device is held
at a different orientation, as shown in FIG. 15C, the fluid 1504 is retained in the
tube 1502 and not allowed to make contact with the outflow channel 1500, which could
allow fluid 1504 to flow back into the device via backflow through the outflow channel
1500. In the examples of FIG. 15C, this retention is achieved because the shape of
the tube tip 1502A and properties of the fluid 1504 are such that surface tension
in the fluid is sufficient to hold the fluid in the tip despite the orientation. In
contrast, in certain examples such as FIG. 15D, surface tension may be insufficient
to prevent gravity from drawing the fluid 1504 out of the tip 1502B and down onto
the side of the tube 1502C, for example when large amounts of fluid have been collected.
In those examples, the channel 1500 is positioned in the tube 1502 such that the fluid
1504 disposed along the side of the tube 1502C does not contact the channel 1500,
thereby preventing backflow out of the tube.
[0101] Further examples of this outflow channel 1500 are contemplated in FIGS16A-E for the
same action and purpose as shown here in FIGS 15A-D. In FIG. 16A, one example features
an outflow channel 1600 A having first 1604 A and second 1606 A channel edges which
are in fluidic connection 1605 A with the inner surface 1607 of the tube 1602A. That
is, the two channel edges 1604A, 1606 A are in contact with the inner surface 1607
such that fluid 1605 that flows out of the outflow channel 1600 A will come in contact
with the inner surface 1607 of the tube 1602A. Thus, when the device and tube 1602A
are substantially upright, the fluid is able to flow out from the outflow channel
1600A and into the tube 1602A, and when it is rotated in the direction of reference
arrow A fluid 1605 is brought into contact with the inner surface 1607A of the tube.
[0102] As is shown in FIG. 16B, an alternative example features an outflow channel 1600B
featuring first 1604B and second 1606B channel edges which are in fluidic connection
1605 A with the top surface 1608 of the tube 1602B such that when the device and tube
are substantially upright, the fluid is able to flow out from the outflow channel
1600B, thereby being brought into contact with the inner surface of the tube 1608.
When the tube is laid down flat (in the direction of reference arrow B), the front
face of the tube thus becomes the top face, and gravity pulls the fluid 1605 down
and away from the outflow channel, thereby preventing fluid flow back into the collector.
[0103] As is shown in FIG. 16C, a bulb-type outflow channel 1600C comprising first1604C
and second 1606C channel edges which form a bulbous shape may be utilized so as to
not connect or physically contact to any edge or surface of the tube 1602C. Instead,
this outflow channel 1600A allows fluid 1605 to drip from the outflow channel 1600C
into the tube 1602C, without a fluidic bridge being formed to the inside of the reservoir
1602C to influence fluid flow. In certain examples not being part of the invention,
notches 1609 at the distal end of these outflow channels can help facilitate droplet
formation and droplet detachment, by weakening surface tension forces in the outflow
channel.
[0104] As is shown in FIG. 16D, a splayed outflow channel 1600D is utilized, wherein the
first 1604D and second 1606D channel edges extend away from one another at the distal
ends. This splayed configuration accommodates fluid drop into the tube 1602D by increasing
the space between the first 1604D and second 1606D channel edges, thereby increasing
the relative role of gravity on the fluid when dripping.
[0105] Finally, in FIG. 16E, a narrow "straight channel" outflow channel 1600E can be employed,
so as to further move the outflow point at the distal end of the channel 1612 away
from the top edge 1620 and inner surface of the tube 1602E. In certain applications,
the example of 16E is preferred, because these examples introduce substantial distance
1610 between the collector and the distal end of the first 1604E and second 1606E
channel edges, which prevents dripping fluid from contacting the inner surface of
the tube 1602E. This distance 1610, along with the narrow shape of the channel 1600E
also reduces the chance of backflow caused by fluidic connection between the fluid
1605 from the outflow channel 1600E and the inner surfaces of the tube 1602E, as increases
in distances between surfaces inhibit fluidic bridging. That is, the distance 1610
between the proximal 1614 and the distal ends 1612 of the channel edges 1604E, 1606E
reduces the chance of a fluidic connection by releasing the fluid 1605 at a distance
apart from both the top edge of the tube 1620 and the top edge of the collecting fluid
1605B, thereby preventing pooling and the creation of fluidic bridges regardless of
the orientation of the channel.
[0106] In FIGS. 17A-B, certain alternative examples of a specific-volume collection device
reservoir 1700 are shown, wherein the reservoir 1700 comprises at least two reservoir
channels 1703, 1705. In this example, the reservoir 1700 has an opening 1701, that
can be coupled to a fluid collector, including any collector disclosed or contemplated
herein. The opening 1701 may be of the same diameter as a standard tube discussed
above in relation to FIGS. 1A-C. In these examples, the reservoir 1700 connects to
a blood collection device in such a way that a fixed receiving feature 1702 extends
into a first reservoir channel 1703 of defined volume. The receiving feature 1702
is thus fixedly disposed along the wall of the reservoir, such that at the proximal
end 1702A it is able to be in fluidic communication with an outflow channel of the
collector 1710, and at the distal end 1702B is able to fill the reservoir 1703.. The
blood being collected is therefore able to contact the outflow channel 1710 more readily
than if it required to contact the surface of the tube. Thus the blood will be guided
by the receiving feature 1702 to the base 1703 A of the first reservoir channel 1703,
thereby allowing the first reservoir channel 1703 to be filled first in sequence.
Once filled, angled features 1704 on the top of the reservoir 1703 guide excess fluid
into a secondary reservoir 1705. The secondary reservoir channel 1705 can thus be
utilized as an overfill reservoir, sequestering the excess blood or as a subsequent
reservoir for blood containment. In alternative examples, multiple reservoirs, such
as three, four, five or more reservoirs can be filled sequentially in this fashion.
[0107] FIG. 17B depicts a top view of the example detailed in FIG. 17A. Importantly, the
second channel 1705 can further comprise a cross-sectional shape that insures efficient
filling, as would be understood by one of skill in the art. For example, an angled
corner 1706 can be placed on the reservoir 1700 such that it has a higher capillary
affinity. In these examples, fluid inputted into the secondary reservoir 1705 through
the angled features 1704 will contact the narrow portion 1708 of the secondary reservoir
1705 and guide the blood to the bottom floor 1705 A of the reservoir, thereby allowing
a robust filling without creating air bubbles.
[0108] In these examples, fluid originating from the collector is drawn into a tube(such
as tube 1700) connected to the device that has multiple cavities or reservoir channels
(such as channels 1703, 1705 discussed above) of known and precise volume, so as to
enable blood collection and analysis in applications that require a specific volume
of fluid. The transfer of blood from the device to the tube (such as tube 1700) is
facilitated by features along the length of the tube on the inner diameter. These
features can be small channels, grooves, or texture that enable capillary guidance
of the fluid into the various reservoirs. For example, a single raised outflow channel
(such as the outflow channel 1702 discussed above) spanning from the top of the tube
to the reservoir can be used to decrease the gap distance between the tube and the
fluid output in the blood collection device as well as guide the fluid along the side
of the tube into the desired reservoir. This protrusion can be of various heights,
such as from 50um up to several millimeters. Similarly, multiple outflow channels
disposed side by side can be used to form an open channel oriented down the side of
the tube and into the reservoir of interest. These features protrude outwards to fit
into an open microfluidic channel in the device, thereby enhancing the contact of
blood from the device to the tube. The blood flows down the tube assisted by the force
of gravity. The features guide the flow along the side of the tube into the appropriate
reservoir, allowing the initial filling of that reservoir to a specific volume. As
discussed above with respect to the tube 1700, once the first reservoir is full, the
subsequent reservoirs are allowed to fill, thereby guaranteeing a set volume in the
specific reservoir or reservoirs. These features can be used to collect a determined
amount of fluid and discard the excess in overfill reservoirs or collect multiple
aliquots of blood in separate reservoirs.
[0109] FIG. 18A depicts an example not being part of the invention of a circular cartridge
reservoir 1900 that can be used with any of the collector examples discussed above.
In these examples, the cartridge 1900 contains a containment region 1901 designed
using open microfluidic principles, thereby allowing the reservoir 1900 to be devoid
of a ceiling, top, or any type of cover. In examples, the region 1901 has a T-shaped
open microfluidic outflow channel 1903 and a protrusion 1902 fluidically connected
thereto. The T-shaped channel 1903 has no "ceiling" and is in fluidic communication
with the microfluidic network of the collector when coupled thereto. FIGS. 18B-C depict
the cartridge protrusion 1902 (FIG. 18B) which establishes the fluidic connection
with the collector (not shown) (FIG. 18C). As best shown in FIG. 18C, this configuration
of the channel 1903 and protrusion 1902 allows for fluid communication with a corresponding
collector protrusion 1906, which in this example is oriented with an inverse T-shape
relative to the protrusion 1902 and channel 1903 on the cartridge 1900 such that the
collector protrusion 1906 is mateable with the protrusion 1902 and channel 1903. The
collector protrusion 1906 therefore contains corresponding open microfluidic channels
1904, 1905 as well. Further, in examples, the cartridge protrusion 1902 and collector
protrusion 1906 can be freely rotated relative to one another, such that they can
be brought into and out of fluidic communication.
[0110] These geometries allow the free motion of one protrusion relative to the other as
the T shape channel allows for such motion. As the collector protrusion 1906 contacts
the cartridge protrusion 1902, blood is able to bridge between the two channels and
flow from one to the other, thereby filling the containment region 1901. Fluidic connections
can be ceased by simply rotating the cartridge, thereby allowing its removal from
the blood collection device.
[0111] Although the disclosure has been described with reference to preferred embodiments,
persons skilled in the art will recognize that changes may be made.